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Modern Engineering Thermodynamics

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720 CHAPTER 17: <strong>Thermodynamics</strong> of Biological Systems<br />

EXAMPLE 17.10 (Continued )<br />

1E−18<br />

1E−19<br />

1E−20<br />

log(k d /a)<br />

1E−21<br />

1E−22<br />

1E−23<br />

1E−24<br />

300 302 304 306 309 311 313 315<br />

Temperature (K)<br />

FIGURE 17.15<br />

Example 17.10, Exercise 30.<br />

One of the most interesting unsolved problems in evolutionary biology is that of biological aging and<br />

development. What determines the beginning and the end of growth? Why do some cells develop into one kind<br />

of organ and other cells into a completely different organ? Also, there is a remarkable similarity between the<br />

following biological groups:<br />

■<br />

■<br />

■<br />

■<br />

■<br />

■<br />

■<br />

The grouping of elements to form active biochemical entities (such as amino acids).<br />

The grouping of these entities to form macromolecules.<br />

The grouping of macromolecules to form cells.<br />

The grouping of cells to form living creatures<br />

(plants and animals).<br />

1.00<br />

The grouping of these living creatures into<br />

productive units (families, industries, etc.).<br />

The grouping of these families into cultures<br />

(or societies).<br />

0.75<br />

The grouping of these cultures into nations.<br />

Recently, West, Brown, and Enquist 1 discovered a single<br />

universal curve that describes the growth of many<br />

diverse species. A plot of a dimensionless mass,<br />

r = ðm/MÞ 1/4 , versus a dimensionless time variable,<br />

τ = ðat/4M 1/4 Þ − ln ½1 − ðm 0 /MÞ 1/4 Š, for a wide variety<br />

of species shows that growth curves for all organisms<br />

fall on the same universal curve r = 1 – e –τ (shown as<br />

a solid line in Figure 17.16), where a is a constant, t is<br />

time, m 0 is the mass at birth (i.e., at t = 0), and M is<br />

the maximum body size. Their model identifies r as<br />

the proportion of total lifetime metabolic power used<br />

for maintenance and other activities and provides the<br />

basis for deriving relationships for growth rates and<br />

the timing of life history events.<br />

Thus, there seems to be a common phenomenological<br />

driving force that is not only responsible for the organization<br />

of molecular structure but is also responsible<br />

for the organization of the cultural bonds of nations<br />

Dimensionless mass ratio, r<br />

0.50<br />

0.25<br />

Data covers shrews, rats, rabbits, pigs, cows, cod,<br />

shrimp, salmon, guppy, robins, hens, and heron.<br />

0 0 2 4 6 8 10<br />

Dimensionless time, τ<br />

FIGURE 17.16<br />

Aplotofthedimensionlessmassratio,r = ðm/MÞ 1/4 , versus<br />

the dimensionless time variable, τ = ðat/4M 1/4 Þ −<br />

ln ½1 − ðm 0 /MÞ 1/4 Š, for a wide variety of species. (Source: Geoffrey<br />

West, James Brown, and Brian Enquist, “A general model for<br />

ontogenetic growth”. Adapted by permission from Macmillan<br />

Publishers Ltd: Nature 413, no. 201, pp. 628–631, copyright 2001.)<br />

1 Nature 413, (October 11, 2001), pp. 628–631.

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